To solve the given differential equation, we notice that it is a first-order linear differential equation of the form:
\[(1 + x^2) \frac{dy}{dx} + y = e^{\tan^{-1}x}.\]We need to make this equation into the standard form:
\[\frac{dy}{dx} + \frac{y}{1 + x^2} = \frac{e^{\tan^{-1}x}}{1 + x^2}.\]The integrating factor (IF) for this equation is given by:
\[IF = e^{\int \frac{1}{1+x^2} \, dx}= e^{\tan^{-1}x}.\]Multiplying the entire differential equation by this integrating factor, we have:
\[e^{\tan^{-1}x}\left(\frac{dy}{dx} + \frac{y}{1 + x^2}\right) = \frac{e^{2\tan^{-1}x}}{1 + x^2}.\]This simplifies to:
\[\frac{d}{dx}\left(ye^{\tan^{-1}x}\right) = \frac{e^{2\tan^{-1}x}}{1 + x^2}.\]Integrating both sides, we have:
\[ye^{\tan^{-1}x} = \int \frac{e^{2\tan^{-1}x}}{1 + x^2} \, dx + C.\]Now, to evaluate the integral, let \(t = \tan^{-1}x\), which implies \(\frac{dt}{dx} = \frac{1}{1+x^2}\) or \(dx = (1 + x^2) \, dt\). Thus, the integral becomes:
\[\int e^{2t} \, dt = \frac{e^{2t}}{2} + C.\]Substituting back, we have:
\[ye^{\tan^{-1}x} = \frac{e^{2\tan^{-1}x}}{2} + C.\]Substituting the initial condition \(y(1) = 0\) when \(x = 1\):
\[0 = \frac{e^{\pi/4}}{2} + C.\]This gives us:
\[C = -\frac{e^{\pi/2}}{2}.\]Substituting C back into the solution, we have:
\[ye^{\tan^{-1}x} = \frac{e^{2\tan^{-1}x}}{2} - \frac{e^{\pi/2}}{2}.\]Therefore, solving for \(y\), we have:
\[y = \frac{e^{\tan^{-1}x}}{2} - \frac{e^{\tan^{-1}x-\pi/2}}{2}.\]To find \(y(0)\), substitute \(x = 0\), which gives:
\[y(0) = \frac{1}{2} - \frac{1}{2} e^{\pi/2}.\]Thus, the value of \(y(0)\) is:
\( \frac{1}{2} \left( 1 - e^{\pi/2} \right) \)
The given differential equation is:
\[ \frac{dy}{dx} + \frac{y}{1+x^2} = \frac{e^{\tan^{-1}x}}{1+x^2}. \]
Integrating factor (I.F.):
\[ \text{I.F.} = e^{\int \frac{1}{1+x^2} dx} = e^{\tan^{-1}x}. \]
Multiply through by I.F.:
\[ y \cdot e^{\tan^{-1}x} = \int e^{\tan^{-1}x} \cdot \frac{e^{\tan^{-1}x}}{1+x^2} dx + C. \]
Simplify:
\[ y \cdot e^{\tan^{-1}x} = \int e^{2\tan^{-1}x} \cdot \frac{1}{1+x^2} dx + C. \]
Substitute:
\[ \tan^{-1}x = z, \quad \frac{1}{1+x^2} dx = dz. \]
Thus:
\[ y \cdot e^{\tan^{-1}x} = \frac{e^{2z}}{2} + C. \]
Apply initial condition: \( y(1) = 0 \), \( \tan^{-1}(1) = \frac{\pi}{4} \):
\[ 0 = \frac{e^{\pi/2}}{2} + C \implies C = -\frac{e^{\pi/2}}{2}. \]
Finally:
\[ y \cdot e^{\tan^{-1}x} = \frac{e^{2\tan^{-1}x}}{2} - \frac{e^{\pi/2}}{2}. \]
At \( x = 0 \), \( \tan^{-1}(0) = 0 \):
\[ y(0) = \frac{1}{2} \left( 1 - e^{-\pi/2} \right). \]
Let $y=y(x)$ be the solution of the differential equation $\left(x^2-3 y^2\right) d x+3 x y d y=0, y(1)=1$.Then $6 y^2( e )$ is equal to
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,